When an air bubble of radius r rises from the bottom to the surface of a lake, its radius becomes 5r/4 Taking the atmospheric pressure to be equal to 10m height of water column, the depth of the lake would approximately be (ignore the surface tension and the effect of temperature):

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Published June 28, 2025
Physics
Fluid Mechanics
Hydrostatics
Gas Laws
Pressure-Volume Relationships

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Detailed Explanation

Key ideas needed

  1. Hydrostatic Pressure
    Water pressure increases with depth: P=Patm+ρghP = P_{\text{atm}} + \rho g h where hh is depth, ρ\rho is water density, and gg is acceleration due to gravity.

  2. Ideal Gas Law in Constant Temperature (Isothermal)
    For a fixed mass of gas at constant temperature: PV=constantP V = \text{constant} A bubble is just a tiny gas packet, so if temperature change is ignored, we can write P1V1=P2V2P_1 V_1 = P_2 V_2

  3. Volume of a Sphere
    V=43πr3V = \frac{4}{3} \pi r^3 Volume is proportional to r3r^3.

Logical chain a student would follow

  • Step 1: Relate pressures at two positions of the bubble (bottom vs. surface).
  • Step 2: Express volumes in terms of the given radii rr and 5r/45r/4.
  • Step 3: Use P1V1=P2V2P_1 V_1 = P_2 V_2 to link pressure and volume, then cancel common factors.
  • Step 4: Insert the known atmospheric pressure (equivalent to 10 m of water) to solve for unknown depth hh.
  • Step 5: Perform quick fraction arithmetic to get an approximate depth.

Each step combines a specific physical principle with a straightforward algebra move, letting you isolate hh efficiently.

Simple Explanation (ELI5)

🫧 Why does the bubble grow?

Imagine you’re holding a balloon deep under water. The deeper you go, the harder the water pushes on it. When you let the balloon float up, that extra push disappears, so the balloon can swell and look bigger.

In this question:

  • At the bottom, the water bubble has size r.
  • At the top (surface), it grows to 5r/4 (that’s a bit bigger than its old size).
  • We know how much the water above pushes (atmospheric pressure is like standing under 10 m of water).

We compare how squeezed the bubble is at the bottom versus the top using a simple rule: "push × space = same number" (that’s the gas law). From that, we can find how deep the bubble started.

It turns out the bubble started roughly 9½ m down.

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Step-by-Step Solution

Step-by-step calculation

  1. Pressures
    Bottom of lake: P1=Patm+ρghP_1 = P_{\text{atm}} + \rho g h
    Surface: P2=PatmP_2 = P_{\text{atm}}

  2. Volumes
    V1=43πr3V_1 = \frac{4}{3}\pi r^3
    V2=43π(5r4)3=43πr3(12564)V_2 = \frac{4}{3}\pi\left(\frac{5r}{4}\right)^3 = \frac{4}{3}\pi r^3\left(\frac{125}{64}\right)

  3. Isothermal condition
    P1V1=P2V2P_1 V_1 = P_2 V_2 (Patm+ρgh)V1=Patm  V1(12564)\bigl(P_{\text{atm}} + \rho g h\bigr) V_1 = P_{\text{atm}} \; V_1 \left(\frac{125}{64}\right) Patm+ρgh=Patm(12564)P_{\text{atm}} + \rho g h = P_{\text{atm}} \left(\frac{125}{64}\right)

  4. Isolate hh
    ρgh=Patm(125641)=Patm(6164)\rho g h = P_{\text{atm}} \left(\frac{125}{64} - 1\right) = P_{\text{atm}} \left(\frac{61}{64}\right)

  5. Insert atmospheric pressure in water-column form
    Given Patm=ρg(10m)P_{\text{atm}} = \rho g (10\,\text{m})
    ρgh=ρg(10)(6164)\rho g h = \rho g (10) \left(\frac{61}{64}\right)
    h=10×61649.53mh = 10 \times \frac{61}{64} \approx 9.53\,\text{m}

Final Answer

The depth of the lake is approximately 9.5m9.5\,\text{m}.

Examples

Example 1

Air bubbles in scuba diving expand as a diver ascends; divers must exhale to avoid lung over-expansion.

Example 2

Deployed life-rafts inflate more at sea level than when packed at depth in a submarine.

Example 3

Weather balloons expand as they rise in the atmosphere where external pressure decreases.

Example 4

Soda bubbles grow when a bottle is opened because external pressure drops suddenly.

Example 5

Deep-sea fish brought up rapidly suffer swim-bladder expansion due to reduced pressure.

Visual Representation

References

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